An effective Hamiltonian for calculating rotational energy levels of an open-shell diatomic molecule, in a 2Sϩ1 ⌺ electronic state, weakly bonded to a closed-shell partner was presented (W. M. Fawzy, J. Mol. Spectrosc. 191, 68 -80 (1998)). The Hamiltonian was given as H ϭ H ev ϩ H rot ϩ H sr ϩ H ss
Dunham Treatment Including Effects of the Born–Oppenheimer Breakdown for Open-Shell Diatomic Molecules in2Σ States
✍ Scribed by Hiromichi Uehara
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 179 KB
- Volume
- 192
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
A Dunham treatment of an effective Hamiltonian for diatomic molecules in 2 ⌺ states that includes contributions of the Born-Oppenheimer breakdown has yielded an expression for vibrational-rotational energy by an expansion in powers of (v ϩ
state and k ϭ 0, 1, . . . , j. Analytic expressions for the expansion coefficients Y* ijk vJ provide a potential model appropriate for the spectral fits for molecules in 2 ⌺ states. The expansion coefficients Y* ij0 vJ for the k ϭ 0 terms are exactly the same as the Y* ij vN coefficients given for 1 ⌺ states, the Dunham coefficients Y ij modified by the contributions of the Born-Oppenheimer breakdown, provided that a spin contribution originating from off-diagonal electronic corrections of the electronic part of the spin-orbit interaction can be ignored. Spin-rotation energy is given by the terms with coefficients Y* ijk vJ (k Ն 1). There are no Y* ijk vJ (k Ն 2) terms in the previously known methods of analysis for 2 ⌺ molecules. The present potential model is applied to the reported vibrational-rotational spectra of CaH and all spectral lines of 40 CaH and 40 CaD isotopomers are fitted to a single set of molecular constants simultaneously with significantly smaller standard deviations.
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